11th And 12th > Mathematics
DIFFERENTIAL EQUATIONS MCQs
Total Questions : 30
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Answer: Option C. ->
sec x = (c + tan x)y
:
C
We have dydx=y tan x−y2sec x⇒1y2dydx−1ytanx=−secx
Putting 1y=v⇒−1y2dydx=dvdx, we obtain
dvdx+tan x.v=secxwhich is linear
I.F=e∫tanxdx=elogsecx=secx
∴ The solution is
v secx=∫sec2xdx+c⇒1ysecx=tanx+c
⇒secx=y(c+tanx)
:
C
We have dydx=y tan x−y2sec x⇒1y2dydx−1ytanx=−secx
Putting 1y=v⇒−1y2dydx=dvdx, we obtain
dvdx+tan x.v=secxwhich is linear
I.F=e∫tanxdx=elogsecx=secx
∴ The solution is
v secx=∫sec2xdx+c⇒1ysecx=tanx+c
⇒secx=y(c+tanx)
Answer: Option D. ->
(2x2−1)x(1−x2)
:
D
x(1−x2)dy+(2x2y−y−ax3)dx=0dydx+(2x2−1)x(1−x2)y=ax2(1−x2),∴P=2x2−1x(1−x2).
:
D
x(1−x2)dy+(2x2y−y−ax3)dx=0dydx+(2x2−1)x(1−x2)y=ax2(1−x2),∴P=2x2−1x(1−x2).
Answer: Option B. ->
f(yx)=cx
:
B
We have, xdy=(y+xf(yx)f′(yx))dx
⇒dydx=yx+f(yx)f′(yx) which is homogenous
Putting y=vx⇒dydx=v+xdvdx, we obtain
v+xdvdx=v+f(v)f′(v)⇒f′(v)f(v)dv=dxx
Integrating, we get log f(v)=logx+logc
⇒logf(v)=logcx⇒f(yx)=cx
:
B
We have, xdy=(y+xf(yx)f′(yx))dx
⇒dydx=yx+f(yx)f′(yx) which is homogenous
Putting y=vx⇒dydx=v+xdvdx, we obtain
v+xdvdx=v+f(v)f′(v)⇒f′(v)f(v)dv=dxx
Integrating, we get log f(v)=logx+logc
⇒logf(v)=logcx⇒f(yx)=cx
Answer: Option A. ->
2x etan−1y,=e2tan−1y+k
:
A
dxdy+11+y2x=11+y2etan−1y
I.F=e∫11+y2dy=etan−1y
∴ Solution is x.etan−1y
=∫etan−1y.11+y2etan−1dy=12e2 tan−1y+12k⇒2x etan−1y=e2 tan−1y+k
:
A
dxdy+11+y2x=11+y2etan−1y
I.F=e∫11+y2dy=etan−1y
∴ Solution is x.etan−1y
=∫etan−1y.11+y2etan−1dy=12e2 tan−1y+12k⇒2x etan−1y=e2 tan−1y+k
Answer: Option B. ->
ny2+x2 =constant
:
B
Differentiating, we have an−1dydx=nxn−1⇒an−1=nxn−1dxdy
Putting this value in the given equation, we have nxn−1dxdyy=xn
Replacing dydxby −dydy, we have ny=−xdxdy
⇒nydy+xdx=0⇒ny2+x2 =constant. Which is the required family of orthogonal trajectories.
:
B
Differentiating, we have an−1dydx=nxn−1⇒an−1=nxn−1dxdy
Putting this value in the given equation, we have nxn−1dxdyy=xn
Replacing dydxby −dydy, we have ny=−xdxdy
⇒nydy+xdx=0⇒ny2+x2 =constant. Which is the required family of orthogonal trajectories.
Answer: Option C. ->
xy+ylogx+x sin y=C
:
C
The given equation can be written as y(1+x−1)dx+(x+logx)dy+sin ydx+xcos ydy=0
⇒d(y(x+logx))+d(xsiny)=0→y(x+logx)+xsiny=C
:
C
The given equation can be written as y(1+x−1)dx+(x+logx)dy+sin ydx+xcos ydy=0
⇒d(y(x+logx))+d(xsiny)=0→y(x+logx)+xsiny=C
Answer: Option A. ->
y=C1e3x+C2e4x
:
A
The given equation can be written as (ddx−3)(dydx−4y)=0....(i)
If dydx−4y=u then (I) reduces to dudx−3u=0
⇒duu=3dx⇒u=C1e3x. Therefore, we have dydx−4y=C1e3x which is a linear equation whose I.F.is e−4x. So ddx(ye−4x)=C1e−x
⇒ye−4x=−C1e−x+C2⇒y=C1e3x+C2e4x
:
A
The given equation can be written as (ddx−3)(dydx−4y)=0....(i)
If dydx−4y=u then (I) reduces to dudx−3u=0
⇒duu=3dx⇒u=C1e3x. Therefore, we have dydx−4y=C1e3x which is a linear equation whose I.F.is e−4x. So ddx(ye−4x)=C1e−x
⇒ye−4x=−C1e−x+C2⇒y=C1e3x+C2e4x
Answer: Option A. ->
c eex22=sin(y−x)
:
A
Put y-x = z. Then dydx−1=dzdx⇒dydx=1+dzdx
Given dydx−x tan(y−x)=1⇒1+dzdx−x tan z=1⇒dzdx=x tan z⇒1tanzdz=x dx⇒∫cotz dz=∫x dx
⇒log|sin z|−logc=x22⇒log|sin zc|=x22=sinzc=ex22⇒sin(y−x)=c ex22
∴ The solution is sin(y−x)=cex22, where c is arbitrary constant.
:
A
Put y-x = z. Then dydx−1=dzdx⇒dydx=1+dzdx
Given dydx−x tan(y−x)=1⇒1+dzdx−x tan z=1⇒dzdx=x tan z⇒1tanzdz=x dx⇒∫cotz dz=∫x dx
⇒log|sin z|−logc=x22⇒log|sin zc|=x22=sinzc=ex22⇒sin(y−x)=c ex22
∴ The solution is sin(y−x)=cex22, where c is arbitrary constant.
Answer: Option B. ->
x3y2+x2y=c
:
B
x2dy−2x3y3dy=3x2y4dx+2xydx⇒x2dy−2xydx=3x2y4dx+2x3y3dy⇒2xydx−x2dyy2+3x2y2dx+2x3ydy=0⇒d(x2y)+d(x3y2)=0⇒x2y+x3y2=C
:
B
x2dy−2x3y3dy=3x2y4dx+2xydx⇒x2dy−2xydx=3x2y4dx+2x3y3dy⇒2xydx−x2dyy2+3x2y2dx+2x3ydy=0⇒d(x2y)+d(x3y2)=0⇒x2y+x3y2=C
Answer: Option A. ->
1
:
A
On Putting x=tanA,y=tanB we get
secA+secB=λ(tanA secB−tanB secA)cosA+cosB=λ(sinA−sinB)tan(A−B2)=1λtan−1x−tan−1y=2tan−11λ
On differentiating 11+x2−11+y2dydx=0
:
A
On Putting x=tanA,y=tanB we get
secA+secB=λ(tanA secB−tanB secA)cosA+cosB=λ(sinA−sinB)tan(A−B2)=1λtan−1x−tan−1y=2tan−11λ
On differentiating 11+x2−11+y2dydx=0